Strain-compensated Ga(AsP)/Ga(AsBi)/Ga(AsP) quantum-well active-region lasers (Conference Presentation)

Author(s):  
Honghyuk Kim ◽  
Yingxin Guan ◽  
Kamran Forghani ◽  
Thomas F. Kuech ◽  
Luke J. Mawst
Keyword(s):  
2012 ◽  
Vol 111 (10) ◽  
pp. 103113 ◽  
Author(s):  
Mikhail V. Kisin ◽  
Chih-Li Chuang ◽  
Hussein S. El-Ghoroury

2015 ◽  
Vol 644 ◽  
pp. 398-403 ◽  
Author(s):  
Tao Lin ◽  
Haoqing Zhang ◽  
Ruijuan Sun ◽  
Yupeng Duan ◽  
Nan Lin ◽  
...  

Nanomaterials ◽  
2021 ◽  
Vol 11 (10) ◽  
pp. 2695
Author(s):  
Chang Liu ◽  
Xuan Zuo ◽  
Shaohui Xu ◽  
Lianwei Wang ◽  
Dayuan Xiong

We propose a stacked dual-band quantum well infrared photodetector (QWIP) integrated with a double-layer gold disk. Two 10-period quantum wells (QW) operating at different wavelengths are stacked together, and gold nano-disks are integrated on their respective surfaces. Numerical calculations by finite difference time domain (FDTD) showed that the best enhancement can be achieved at 13.2 and 11.0 µm. By integrating two metal disks, two plasmon microcavity structures can be formed with the substrate to excite localized surface plasmons (LSP) so that the vertically incident infrared light can be converted into electric field components perpendicular to the growth direction of the quantum well (EZ). The EZ electric field component can be enhanced up to 20 times compared to the incident light, and it is four times that of the traditional two-dimensional hole array (2DHA) grating. We calculated the enhancement factor and coupling efficiency of the device in the active region of the quantum well. The enhancement factor of the active region of the quantum well on the top layer remains above 25 at the wavelength of 13.2 μm, and the enhancement factor can reach a maximum of 45. Under this condition, the coupling efficiency of the device reaches 2800%. At the wavelength of 11.0 μm, the enhancement factor of the active region of the quantum well at the bottom is maintained above 6, and the maximum can reach about 16, and the coupling efficiency of the device reaches 800%. We also optimized the structural parameters and explored the influence of structural changes on the coupling efficiency. When the radius (r1, r2) of the two metal disks increases, the maximum coupling efficiency will be red-shifted as the wavelength increases. The double-layer gold disk structure we designed greatly enhances the infrared coupling of the two quantum well layers working at different wavelengths in the dual-band quantum well infrared photodetector. The structure we designed can be used in stacked dual-band quantum well infrared photodetectors, and the active regions of quantum wells working at two wavelengths can enhance the photoelectric coupling, and the enhancement effect is significant. Compared with the traditional optical coupling structure, the structure we proposed is simpler in process and has a more significant enhancement effect, which can meet the requirements of working in complex environments such as firefighting, night vision, and medical treatment.


2000 ◽  
Vol 180 (1) ◽  
pp. 275-280 ◽  
Author(s):  
S.V. Ivanov ◽  
A.A. Toropov ◽  
T.V. Shubina ◽  
S.V. Sorokin ◽  
O.V. Nekrutkina ◽  
...  

1993 ◽  
Vol 127 (1-4) ◽  
pp. 46-49 ◽  
Author(s):  
M.L. Dotor ◽  
J. Meléndez ◽  
P. Huertas ◽  
A. Mazuelas ◽  
M. Garriga ◽  
...  

1992 ◽  
Vol 281 ◽  
Author(s):  
J. Lopata ◽  
N. K. Dutta ◽  
Naresh chand

Strained layer In0.2Ga0.8As/GaAs quantum-well (QW) lasers have been used to pump Erbium Doped Fiber Amplifiers for use in opto-electronic communication systems. These InGaAs/GaAs Q-W lasers grown as graded index separate confinement heterostructures (GRINSCH) emit at 980 nm and have exhibited low threshold current densities, high electrical to optical power conversion efficiencies, low noise, and low temperature sensitivities [1–3]. Recently there has been much attention toward the growth and fabrication of devices containing short period superlattices of (InAs)m/(GaAs)m or (GaAs)m/(AlAs)n compositions [4–9]. Indeed the growth of inverted MODFET structures using a (GaAs)/(AlAs) superlattice barrier in place of an AlGaAs random alloy exhibited an increase in low temperature mobility due to reductions in the number of impurities and interface roughness [7]]. Can the optical properties of strained layer InGaAs/GaAs Q-W lasers also be improved by growing an (InAs)/(GaAs)4 short period superlattice as the active layer in place of the In0.2Ga0.8 As random alloy?This paper reports the fabrication of ridge waveguide lasers using a 6 period (InAs)1/(GaAs)4 superlattice active region in a GRINSCH laser structure. One period of the superlattice consists of 1 monolayer (ML) of InAs and 4 ML of GaAs. Thus the average In composition in the superlattice is 20%. This superlattice laser is an alternative to the In0.2Ga0.8As/GaAs random alloy quantum-well laser used as a pump source for Erbium Doped Fiber Amplifiers. In a single quantum well In0.2Ga0.8As/GaAs laser the active region is a thin layer (-70Å thick) sandwiched between GaAs barrier layers. The superlattice active laser reported here has 6 periods of (InAs)1/(GaAs)4 as the light emitting region of a total width comparable to a single quantum well of random alloy composition.


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